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Quantum Optics II Cozumel, Mexico , December 5-8, 2004. ”Entanglement in Time and Space” J.H. Eberly, Ting Yu, K.W. Chan, and M.V. Fedorov University of Rochester / Prokhorov Institute

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slide1

Quantum Optics II

Cozumel, Mexico, December 5-8, 2004

  • ”Entanglement in Time and Space”
  • J.H. Eberly, Ting Yu, K.W. Chan, and M.V. Fedorov
  • University of Rochester / Prokhorov Institute
  • We consider entanglement as a dynamic property of quantum states and examine its behavior in time and space. Some interesting findings: (1) adding more noise helps fight phase-noise disentanglement, and (2) high entanglement induces spatial localization, equivalent to a quantum memory force.
  • Ting Yu & JHE, Phys. Rev. Lett. 93, 140404 (2004).
  • K.W. Chan, C.K. Law and JHE, Phys. Rev. Lett. 88, 100402 (2002)
  • JHE, K.W. Chan and C.K. Law, Phil. Trans. Roy. Soc. London A 361, 1519 (2003).
  • M.V. Fedorov, et al., Phys. Rev. A 69, 052117 (2004).
slide2

Superposition of conflicting information, but only one object.

Can you handle the conflictinginformation here? Which face is in the back?

Entanglement means a superposition of conflicting information about two objects.

slide3

A pair of conflicts can be “entangled”

Try to see both at the same time.

Do they “flip” together?

slide4

Measurement cancels contradiction

A pair of boxes, but only one view of them

slide5

Bell States provide a simple example

Schrödinger-cat “Bell State”:

|-> =|C*>|N*> + |C>|N>

excited cat = C*, dead cat = C,

excited nucleus = N*, ground state = N

slide6

Bell States provide a simple example

Schrödinger-cat “Bell State”:

|-> =|C*>|N*> + |C>|N>

excited cat = C*, dead cat = C,

excited nucleus = N*, ground state = N

<N|-> = |C> (sorry, Cat)

slide7

Overview

Issue-- entanglement in time and space.

Illustration #1 -- two atoms are excited and entangled but not communicating with each other. Result #1-- both atoms decay, diag e-2gt and off-diag e-gt , just as expected; but entanglement of the atoms behaves qualitatively differently.

Illustration #2 -- two atoms fly apart in molecular dissociation. Result #2-- entanglement means localization in space (a “quantum memory force”).

For detailed treatments:

Ting Yu & JHE, PRL 93 140404 (2004), and M.V. Fedorov, et al., PRA 69, 052117 (2004).

slide8

A B

HAT = (1/2)wAsZA + (1/2)wBsZB , HCAV = kwkak†ak + knkbk†bk

HINT = k(gk*s-Aak† + gks+Aak) + k(fk*s-Bbk† + fks+Bbk)

At t=0 the joint initial state rABis entangled and mixed (not pure). The atoms only decay (no cavity feedback). After t=0, what happens to entanglement?

Illustration #1:

slide9

++ +- -+ --

++ a 0 0 0

+- 0 1 1 0

-+ 0 1 1 0

-- 0 0 0 d

Initial state, entangled and mixed, where d = 1-a.

r =

C = concurrence

EOF concurrence

1 ≥ C ≥ 0

mixedinitial states, C = 2/3

slide10

a(t) 0 0 0

0 b(t) z(t) 0

0 z*(t) c(t) 0

0 0 0 d(t)

r =

a 0 0 0

0 1 1 0

0 1 1 0

0 0 0 d

Time Evolution Result:

Obvious point: the atoms go to their ground states, so d  3, and the other elements decay to zero.

No surprise: the decay of r(t) is smooth, and exponential, measured by usual natural lifetime:

s±A(t) = s±A(0) exp[-GAt/2 ± iwAt]

Reminder: the atoms decay independently.

slide11

(t) =  Km(t) r(0) Km†(t)

Sol’n. in Kraus representation:

Kraus operators:

gA = exp[-Gt / 2 ] wA2 = 1- exp[-Gt ] , same for B.

for details, see Ting Yu and JHE, PRB 68, 165322 (2003)

slide12

r

Decays all depend on gA(t) = exp(-GAt/2) and gB(t) = exp(-GBt/2).

a(t) = gAgB, b(t) = gB2 +gA2 B2, c(t) = gA2 +gB2 A2,

d(t) = A2 +A2 +A2A2, z(t) = gAgB , where A2 = 1 - gA2, etc.

a 0 0 0

0 b z 0

0 z* c 0

0 0 0 d

Usual Born-Markov solutions for the separate atoms:

s±A(t) = s±A(0) exp[-GAt/2 ± iwAt]

Kraus matrix evolution:

For detailed treatment: Ting Yu & JHE, PRL 93, 140404 (2004).

slide13

Entanglement evolution:

Entanglement has its own rules, and follows the atom decay law only exceptionally.

Entanglement can be completely lost in a finite time!

art by Curtis Broadbent

Ting Yu & JHE, Phys. Rev. Lett. 93, 140404 (2004).

slide14

Noise + Entanglement

Werner state density matrix

Werner qubits undergo only off-diagonal relaxation under the influence of phase noise.

All entanglement of a Werner state is destroyed in a finite time by pure phase noise.

slide15

Two Noises + Entanglement

Pure off-diagonal relaxation of qubits

Add some diagonal relaxation, for example via vacuum fluctuations.

Add diag. to off-diag. relaxation of qubits

Werner entanglement gets some protection from added noise!

Ting Yu & JHE (in preparation).

slide16

Experiments following the original EPR “breakup” scenario have

not been done yet.

Spatial localization and entanglement

With just two objects, high entanglement can be reached by allowing each object a wide variety of different states.

The idealized two-particle wave function used by Einstein, Podolsky and Rosen in their famous 1935 EPR paper used continuous variables (infinite number of states) to get the maximum degree of entanglement.

slide17

Spontaneous emission(K ≈ 1)

Chan, Law and Eberly, PRL 88, 100402 (2002)

Fedorov, et al. (in preparation, 2004)

Raman scattering(K > 100)

Chan, Law, and Eberly, PRA 68, 022110 (2003)Chan, et al., JMO 51, 1779 (2004).

Ionization/Dissociation(K > 10)

Fedorov, et al., PRA 69, 052117 (2004).

Chan and Eberly, quant-ph 0404093

Down conversion (K ≈ 4.5 — 1000’s)Huang and Eberly, JMO 40, 915 (1993)

Law, Walmsley and Eberly, PRL 84, 5304 (2000)Law and Eberly, PRL 92, 127903 (2004)

Physical examples of breakup

17

slide18

EPR system is created by break-up

The variables entangled are positions (x1and x2), or momenta (k1 and k2). Perfect correlation is implied in the EPR wavefunction:

How much correlation is realistic? How to measure it?

Original paper: Einstein, Podolsky and Rosen, Phys. Rev. 47, 777 (1935).

slide19

All information is in Y. We can plot the two-particle density |Y|2 vs. x1 and x2.

  • Knowledge of one particle gives information about the other particle.
  • Joint localization information is packet entanglement.

|Y|2

Fedorov ratios

for particle localization:

We can calculate these for a simple dissociation model.

Localization - Entanglement

slide20

relative part

CM part

Time-dependent EPR example

Given a dissociation rategd, a post-breakup diatomicYis:

M.V. Fedorov, et al., PRA 69, 052117 (2004) / quant-ph/0312119.

slide22

Dynamics of localization

What do we know and when do we know it?

  • Massive particles  spreading wavepackets:

Dx Dx(t) and DX DX(t)

  • EPR pairs: [x, P] = 0 and [X, p] = 0 nonlocality
  • Spreading is governed by the free-particle Hamiltonian.
  • Time evolution is merely via phase in the momentum picture:
slide23

Calculation

Inferred dependence

Dynamics of localization - F ratios

Plots of |Y(t)|2

vs. x1 and x2 :

Experiments track localization via packet spreading (i.e.,spatial variances). The two-particle ratio h(t) = ∆x/2∆X is a convenient parameter [*]connected with dynamical evolution.

* Chan, Law and Eberly, PRL 88, 100402 (2002).

slide24

Universal man-in-street theory

Model thebreakup state as double-Gaussian [*].

* K.W. Chan and JHE, quant-ph 0404093

This makes it easy to calculate the Fedorov ratios (F1 ~ F2 )

at t=0 and for later times.

Question: can we guess what happens to localization?

slide25

When these exponents are added, the nonseparablex1x2term  0 at a specific time t0:

Entanglement migration to phase

Therefore P(x, X; t) = (x, X; t)2has two similar real exponents.

slide26

Quantum memory force (QMF)

Atom Photon

The dissociation example has a close analog in spontaneous emission. These atom-photon space functions show a “force” arising from shared quantum information, a “quantum memory force” (QMF).The first four bound states are shown for Schmidt number K = 3.5, which is slightly “beyond-Bell.,” i.e., K > 2. M.V.Fedorov, et al. (in preparation).

Chan-Law-Eberly, PRL 88, 100402 (2002)

slide27

Summary / dynamics of entanglement

  • Entanglement dynamics are largely unknown (time or space)
  • Noisy environment kills entanglement but not intuitively
  • Individual atom decay is not a guide for entanglement
  • Diag. + off-diag. noise has a cancelling effect
  • EPR-type breakup is ubiquitous / creates two-party correlation
  • Conditional localization vs. entanglement ?
  • Packet dynamics, Fedorov ratio and control parameter h
  • Man-in-street theory and phase entanglement
  • Memory effects enforce spatial configurations (QMF)
slide28

Acknowledgement

Research supported by NSF grant PHY-00-72359, MURI Grant DAAD19-99-1-0215, NEC Res. Inst. grant, and a Messersmith Fellowship to K.W. Chan.

References

Ting Yu & J.H. Eberly, PRL 93, 140404 (2004) and in preparation.

M.V. Fedorov, et al., PRA 69, 052117 (2004).

C.K. Law and J.H. Eberly, PRL 92, 127903 (2004).

M.V. Fedorov, et al., PRA (in preparation).

K.W. Chan, C.K. Law and J.H. Eberly, PRL 88, 100402 (2002).

K.W. Chan and J.H. Eberly, quant-ph/0404093.

A. Einstein, B. Podolsky and N. Rosen, Phys. Rev. 47, 777 (1935).

slide29

Size of ent.

More sophisticated Schmidt analysis

Any bipartite pure state can be

written as a single discrete sum:

  • Continuous basis discrete basis
  • Unique association of system 1 to system 2

e.g.,

slide30

Discretization of continuum information,

the Schmidt advantage

Unique

mode pairs

Continuous-mode basis

Schmidt-mode basis

Pure-state non-entropic measure of entanglement:

Schmidt number counts experimental modes, provides practical metric

slide31

Interpreting K, the Schmidt number

K = 1, no entanglement.

K = 2, perfect Bell states.

K = 5, beyond Bell, more information.

K = 10, still more info.

Quantum info is always

discrete and countable.

slide32

Estimation of K for photodissociation

Comparing the photodissociation process with the double-Gaussian model, we identify Dx0 = v ⁄ gd andDX0 = DR0.

If we take DR0 = 10 nm, ,

and define td = gd-1, then with td in sec,

slide33

Retreat of entanglement into phase

The Fedorov ratios for double-Gaussian :

Position:

Momentum:

where

, so .

Note non-equivalence of k-space and x-space

for these experimentally measurable quantities.

slide35

Double-Gaussian Schmidt analysis

For the man-in-street double-Gaussian model (with m1 = m2)

The Schmidt modes are the number states

and one finds:

while from the actual wave function we had inferred

with h(t) = ∆x(t)/2∆X(t). These are the same, except for spreading!

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